Rubidium (Z=37)
76Rb 77Rb 78Rb 79Rb 80Rb 81Rb 82Rb 83Rb 84Rb 85Rb 86Rb 87Rb 88Rb 89Rb 90Rb 91Rb 93Rb 94Rb 95Rb 96Rb 97Rb
Recommended† magnetic dipole moments
Isotope Energy [keV] t1/2 Spin/Parity μ [nm] Method Recommended Tables
82Rb 0 1.26 m 1+ +0.554403(16) ABLS INDC(NDS)-0794
69 6.47 h 5- +1.5096(11) AB INDC(NDS)-0794
192 12.3 ns 6+ +4.02(5) TDPAD INDC(NDS)-0816
3029 0.40 ps 12- (+)13(3) TF INDC(NDS)-0816
3501 0.41 ps 13- (+)13(3) TF INDC(NDS)-0816
4049 0.24 ps 14- (+)12(3) TF INDC(NDS)-0816
4717 <0.7 ps 15- (+)12(3) TF INDC(NDS)-0816


Recommended† electric quadrupole moments
Isotope Energy [keV] t1/2 Spin/Parity Q [b] Method Recommended Tables
82Rb 0 1.26 m 1+ +0.23(10) ABLS INDC(NDS)-0833
69 6.47 h 5- +1.22(27) ABLS INDC(NDS)-0833


Compiled‡ magnetic dipole and electric quadrupole moments from published articles
Isotope Energy [keV] t1/2 Spin/Parity μ [nm] Q [b] Ref. Std Method NSR keyword doi
82Rb 0. 1.25 m 1+ +0.5545083(11) [87Rb] ABLS 1986DU16
1981TH04		 10.1051/jphys:0198600470110190300
10.1103/PhysRevC.23.2720
+0.554(6) OP/RD , R 1978EK04 10.1016/0375-9474(78)90515-8
+0.23(10) [85Rb] 1981TH04
2013STZZ		 10.1103/PhysRevC.23.2720
~100. 6.47 h 5- +1.5100082(2) [87Rb] AB 1976FU06
1957HU75		 10.1063/1.555544
10.1103/PhysRev.107.723
+1.513(2) [87Rb] ABLS 1981TH04 10.1103/PhysRevC.23.2720
+1.51(2) [85Rb] AB , R 1978EK04 10.1016/0375-9474(78)90515-8
+1.2(3) [85Rb] 1981TH04
2013STZZ		 10.1103/PhysRevC.23.2720
191. 12.3 ns 6+ +4.02(5) TDPAD 1996IO01 10.1007/s002180050122
3027. 0.6 ps 12- (+)13(3) TF 2010YU03 10.1088/1674-1056/19/6/062701
3500. 0.6 ps 13- (+)13(3) TF 2010YU03 10.1088/1674-1056/19/6/062701
4048. 0.4 ps 14- (+)12(3) TF 2010YU03 10.1088/1674-1056/19/6/062701
4716. <1 ps 15- (+)12(3) TF 2010YU03 10.1088/1674-1056/19/6/062701

† Recommended magnetic moments are for the bare nucleus with published results corrected consistently for diamagnetism (including error estimate).
  Where appropriate published results are also adjusted to the most recent adopted half-life for the state.
  Recommended quadrupole moments are adjusted using the best electric field gradient calculation for the system concerned.
  For details see the Reports referenced.

‡ In this listing published results are given without adjustment or correction.